共查询到19条相似文献，搜索用时 171 毫秒
1.
利用地基毫米波雷达进行云参数及云内湍流特性的探测和反演。根据云雷达回波的功率谱数据,反演出大气垂直运动速度和云微物理参数,得到云内湍流耗散率ε的大小和分布情况,并进一步研究和分析了云内空气垂直运动与云微物理参数、反射率因子、多普勒速度、速度谱宽变化的关系,更好地了解云的演变情况。对2016年8月8日四川稻城的一次层状云过程的探测和反演表明：1）粒子有效半径随着上升气流的增强而增大,由于碰并聚合的作用,粒子数浓度也呈现相应减小的趋势。2）云内湍流耗散率ε在云底、云顶较大,云内较小,量级在10-8~10-2 m2·s-3,多普勒速度能谱验证了假设雷达探测湍涡的尺度在惯性副区的合理性。3）随着上升气流的增强,云粒子的下沉运动相应减小,速度谱宽相应增大。 相似文献
2.
本文采用RBLM-chem模式,利用杭州市高分辨率城市建筑等资料,定量分析城市动力效应、热力效应以及城市植被、人为热对SO2、NO2、O3、PM2.5等主要污染物浓度的影响。结果表明,城市化过程使得大部分城区温度上升约1℃,相对湿度下降约6%,风速下降约0.8 m·s-1,湍流动能增强约0.03 m2·s-2。城市动力效应主要通过降低城市风速,使得城区污染物浓度升高,SO2浓度有近5 μg·m-3的上升,PM2.5、O3浓度也有近15 μg·m-3的上升。城市热力效应主要通过热岛环流使城区污染物向上输送,令地面污染物浓度降低,在城市大部分区域PM2.5都有大约10 μg·m-3的浓度下降。城市动力效应大于热力效应,城市的总体作用是使污染物浓度升高。城市下垫面使污染物浓度上升的另外一个机制是代替了自然有植被的下垫面,使污染物干沉降速度下降,但这一作用小于动力学效应。另一方面,人为热对城市主要污染物浓度都起着减小的作用,其中SO2、NO2、O3、PM2.5浓度降幅分别在2.5、3.0、6.0、10.0 μg·m-3左右。城市植被可以显著增加污染物干沉降速度,使主要污染物SO2、NO2、O3和PM2.5的干沉降速度分别上升0.1、0.1、0.03、0.06 m·s-1左右,相应地使上述污染物浓度分别下降2.5、6.0、4.0、6.0 μg·m-3左右。 相似文献
3.
锡林浩特草原CO2通量特征及其影响因素分析 总被引：1，自引：0，他引：1
利用锡林浩特国家气候观象台开路涡度相关系统、辐射土壤观测系统,测得的长期连续通量观测数据,对锡林浩特草原2009—2011年期间的CO2通量观测特征进行了分析。结果表明:CO2通量存在明显的年际、季节和日变化特征。3 a中NEE年际变率达到200 g·m-2,季节变率最大达到460 g·m-2,日变化幅度生长季最大达到0.25 mg·m-2·s-1。通过不同时间尺度碳通量与温度、水分、辐射等环境因子的分析,认为CO2通量日变化主要受温度和光合有效辐射影响,而季节变化和年变化主要受降水和土壤含水量的影响。降水强度及时间分布是制约牧草CO2吸收的关键因素,大于15%的土壤含水量有利于促进牧草生长。 相似文献
4.
5.
本试验以PAR （光合有效辐射）800 μmol·m-2·s-1，温度25℃为对照（CK），设置6个处理[L1T1（PAR 200 μmol·m-2·s-1，4℃）、L1T2（PAR 200 μmol·m-2·s-1，6℃）、L1T3（PAR 200 μmol·m-2·s-1，8℃）、L2T1（PAR 400 μmol·m-2·s-1，4℃）、L2T2（PAR 400 μmol·m-2·s-1，6℃）和L2T3（PAR 400 μmol·m-2·s-1，8℃）]，分别处理6、12、24、48和72 h，以研究低温弱光双重胁迫对番茄苗期干物质分配以及不同器官的可溶性糖、可溶性蛋白和游离氨基酸含量的影响.结果表明：低温弱光双重胁迫使地下部分干物质分配比例减小，而对地上部分干物质分配比例无显著影响，地下部分的干物质分配比例随时间的变化与地上部分相反；低温弱光胁迫显著降低了番茄茎和叶片的可溶性糖、可溶性蛋白和游离氨基酸的含量；根的可溶性糖含量随胁迫时间的变化趋势与地上部分不一致，但根、茎、叶片的可溶性糖含量均以L2T3处理72 h含量最高，分别为94.88、77.09和41.62 mg·g-1；根的可溶性蛋白含量随胁迫时间的变化趋势与地上部分不一致，茎和叶片的可溶性蛋白含量均以L2T3处理12 h最高，以L1T1处理72 h最低；不同器官的游离氨基酸含量随胁迫时间的变化趋势与可溶性蛋白相反；弱光对番茄干物质和营养物质含量的影响小于低温.研究证实苗期番茄在低温弱光胁迫前期，干物质和营养物质先向地上部分分配，胁迫24 h后则更多地向根系积累. 相似文献
6.
R. Vogt A. Christen M. W. Rotach M. Roth A. N. V. Satyanarayana 《Theoretical and Applied Climatology》2006,84(1-3):117-126
Summary In Summer 2002 eddy covariance flux measurements of CO2 were performed over a dense urban surface. The month-long measurements were carried out in the framework of the Basel Urban
Boundary Layer Experiment (BUBBLE). Two Li7500 open path analysers were installed at z/zH = 1.0 and 2.2 above a street canyon with zH the average building height of 14.6 m and z the height above street level. Additionally, profiles of CO2 concentration were sampled at 10 heights from street level up to 2 zH. The minimum and maximum of the average diurnal course of CO2 concentration at 2 zH were 362 and 423 ppmv in late afternoon and early morning, respectively. Daytime CO2 concentrations were not correlated to local sources, e.g. the minimum occurred together with the maximum in traffic load.
During night-time CO2 is in general accumulated, except when inversion development is suppressed by frontal passages. CO2 concentrations were always decreasing with height and correspondingly, the fluxes – on average – always directed upward.
At z/zH = 2.2 low values of about 3 μmol m−2 s−1 were measured during the second half of the night. During daytime average values reached up to 14 μmol m−2 s−1. The CO2 fluxes are well correlated with the traffic load, with their maxima occurring together in late afternoon. Daytime minimum
CO2 concentrations fell below regional background values. Besides vertical mixing and entrainment, it is suggested that this
is also due to advection of rural air with reduced CO2 concentration. Comparison with other urban observations shows a large range of differences among urban sites in terms of
both CO2 fluxes and concentrations.
Present affiliation: Swiss Federal Office for Meteorology and Climatology, MeteoSwiss, Zürich, Switzerland 相似文献
7.
基于2016年11月24日—12月23日南京市草场门站、鼓楼站和仙林站的强化试验观测资料,分析了城市和郊区主要大气污染物的时空变化特征及其与气象要素的相互关系。研究发现：观测期间南京PM2.5、PM10、NO2、O3、CO、SO2月均质量浓度分别为52.84~84.34 μg·m-3、88.36~120.34 μg·m-3、49.98~51.66 μg·m-3、24.85~50.57 μg·m-3、0.99~1.2 mg·m-3和22.1~26.48 μg·m-3;近地面,城市大气污染物质量浓度高于郊区,其中城市O3比郊区高61.0%;在城市地区,除NO2和CO外,鼓楼站大气污染物质量浓度高于草场门站,其中鼓楼站PM2.5比草场门站高42.7%;PM2.5小时质量浓度最大为210.93 μg·m-3,重污染过程出现时风速较低、温度较高,郊区PM10、PM2.5、NO2质量浓度呈现高值时的最频风向为南风,O3和SO2质量浓度呈现高值时的最频风向分别为西风和西南风,所以郊区大气污染受城市输送影响。利用HYSPLIT模式研究发现12月4—8日和16—20日的污染气团分别来自西部和北方地区,聚类分析发现12月影响南京市的污染气团45%来自西部地区且移动速度较快,55%来自北方地区且移动速度较慢。由此可见,南京市冬季出现的大气污染,其形成不仅与本地排放和局地气象条件有关,而且西部和北方地区的远距离输送也会造成影响。 相似文献
8.
自2014年以来,中国细颗粒物（PM2.5）浓度大幅度下降,但臭氧（O3）浓度逐年缓慢上升,厘清PM2.5和O3（P-O）相关性尤为关键.在本研究中,2014—2019年北京和南京PM2.5年均质量浓度下降幅度分别为-6.86和-6.15 μg·m-3·a-1;而日最大8小时平均O3质量浓度（MDA8 O3）年均增长幅度为1.50和1.75 μg·m-3·a-1.研究期间,北京地区MDA8 O3质量浓度小于100 μg·m-3,P-O呈负相关;而当质量浓度大于100 μg·m-3时,P-O为正相关.通过Pearson相关系数研究P-O两者相关性.在两个城市每月相关性分析中,在每日时间尺度5—9月为强的正相关;而小时时间尺度11月至次年2月趋于负相关.在北京,P-O每月和季节相关性变化大于南京.在日变化中,夏季在16时为强的正相关,春秋两季在13—17时为弱的正相关,而在春、秋和冬季8时,却为强的负相关. 相似文献
9.
Summary The open-path eddy covariance (EC) method often shows unlikely downward CO2 fluxes in late winter and early spring over drained paddy fields with few active plants. To understand why, we carried out
intensive measurements in a bare paddy field from 9 to 11 April 2003, simultaneously using open- and closed-path EC methods;
aerodynamic and dynamic closed-chamber methods were also used. During this period, the open-path EC method showed downward
daytime CO2 fluxes ranging from 0 to −5.9 μmol m−2 s−1, even after application of the WPL correction (density correction) and ordinary quality control tests. Because the closed-path
EC and aerodynamic methods showed upward CO2 fluxes, the downward CO2 fluxes observed with open-path EC appear not to represent true CO2 transport. Diurnal variations in the downward daytime CO2 fluxes appeared to be correlated with increases in solar radiation during the day, and also with increases in sensible heat
flux in weak winds but not under strongly windy conditions. The daytime 10-Hz time series data of vertical wind and CO2 mixing ratio demonstrated that updrafts were CO2 depleted in the open-path system, whereas the same updrafts were CO2 enriched in the closed-path system. Careful examination of the discrepancies between the open- and the closed-path EC measurements
revealed that the amplitudes of the 10-Hz temperature signals from the sonic anemometer and the resultant sensible heat fluxes
were too small to compensate for the discrepancies observed during the daytime. The open-path EC method with the conventional
application of the WPL correction is not necessarily appropriate for measuring small magnitudes of CO2 flux (≤5 μmol m−2 s−1) under such surface and atmospheric conditions that the magnitude of the WPL correction is as great as that of the uncorrected
CO2 flux itself.
Author’s addresses: Keisuke Ono, 3-1-3 Kannondai, Tsukuba, Ibaraki 305-8604, Japan; Akira Miyata, Tomoyasu Yamada, National
Institute for Agro-Environmental Sciences, Tsukuba, Japan 相似文献
10.
以3个花生品种（开农49号、64号和69号）为材料,通过大田模拟试验,研究UV-B辐射增强对花生结荚期叶片的净光合速率（Pn）、气孔导度（Gs）、胞间CO2浓度（Ci）、蒸腾速率（Tr）和水分利用效率（Ewu）日变化的影响,为筛选高产、抗旱、抗UV-B辐射花生品种提供依据.UV-B辐射设2个水平即自然光（CK,1.5 kJ·m-2）和UV-B增强20%（T,1.8 kJ·m-2）.结果表明,UV-B辐射增强明显抑制花生的光合作用和蒸腾作用,与对照相比,UV-B增强条件下,开农49号、64号和69号Pn日均值分别降低19.4%、27.8%、24.7%;Gs日均值降低26.7%、42.9%、28.6%;Ci日均值降低27.2%、20.4%、23.1%;Tr日均值降低17.8%、23.3%、25.1%;Ewu日均值降低16.6%、23.2%、23.9%.UV-B辐射增强对3个品种生长都具有抑制效应,但品种间存在一定的敏感性差异,其中开农49号最不敏感,因此,开农49号在抗UV-B辐射方面比其他2个品种具有更大的优势. 相似文献
11.
卫星反演海面风场资料能够弥补海上气象测风资料缺乏的不足,对近海风能资源评估具有重要意义。通过ASCAT(Advanced Scatterometer)风速数据与美国及中国近海岸浮标测风资料的对比分析,结果表明,ASCAT风速的均方根误差为1.27 m·s-1。比较利用近海岸浮标逐小时风速及与其相匹配ASCAT瞬时风速计算的各项风能参数,得出ASCAT与浮标的平均风速和风功率密度的残差分别在±0.5 m·s-1和±50 W·m-2以内,该残差占浮标计算结果的比例分别在±8%和±12%以内。使用ASCAT风速资料拟合的Weibull分布函数与浮标的结果较吻合。因此,ASCAT风速资料也能够为海上风能资源评估提供有用的风能参数信息。最后使用ASCAT瞬时风速数据分析了中国近海10 m及70 m高度处的风能资源的空间分布特征,结果表明,台湾海峡平均风速和风功率密度最大。 相似文献
12.
环境场对西北太平洋热带气旋快速增强过程的影响 总被引：5，自引：5，他引：0
利用美国联合台风预警中心整编的西北太平洋1970—2012年热带气旋(TC)最佳路径数据集及ERA-Interim再分析资料,利用极端天气法确定TC快速增强(RI)的阈值为30 kn,分析了快速增强(RI)TC的时空分布特征;从RI的样本中选取9个个例,采用动态合成分析法,对TCRI过程的环境场进行比分析。研究表明:(1)菲律宾群岛以东(10~15°N,130°E)海域为RI发生频数最多的区域,南海地区发生RI的情况明显偏少。(2)RI在1972年发生的概率最大,而在2005年发生的概率最小,1997年后,RI发生的概率波动性较大。(3)西风与西南风水汽输送结合150h Pa附近的反气旋强辐散作用,有利于TCRI过程的进行。(4)RI发生前24 h至RI发生后的6 h,TC中心附近区域平均东风切变较快增大,其值由0.5 m·s~(-1)增加到2.5 m·s~(-1)左右,之后保持在2.0~3.0 m·s~(-1),使TC处于一个有利于其RI过程的纬向风切变环境。 相似文献
13.
苏州城区大气边界层低空急流特征分析 总被引：1，自引：0，他引：1
利用2012年苏州城区风廓线雷达的观测资料,从低空急流个例分析入手,选取1、4、7、10月四个典型月份,分析该地区边界层低空急流的时空分布及强度变化特征。结果表明:冬春两季低空急流发生频率最高,夏季出现频率最低。在4个典型月份里低空急流均表现出日落后出现频率升高,夜间保持稳定,日出后出现频率降低的特征。全年有80%的低空急流分布在900 m以下高度上,冬、夏季平均高度最低。全年低空急流风速70%以上集中在4~12 m·s~(-1),小于4 m·s~(-1)和大于20 m·s~(-1)的低空急流出现频率较低。 相似文献
14.
The Monin–Obukhov similarity theory (MOST) functions fε and fT, of the dissipation rate of turbulent kinetic energy (TKE). ε, and the structure parameter of temperature, CT2, were determined for the stable atmospheric surface layer using data gathered in the context of CASES-99. These data cover
a relatively wide stability range, i.e. ζ=z/L of up to 10, where z is the height and L the Obukhov length. The best fits were given by fε = 0.8 + 2.5ζ and fT= 4.7[ 1+1.6(ζ)2/3], which differ somewhat from previously published functions. ε was obtained from spectra of the longitudinal wind velocity
using a time series model (ARMA) method instead of the traditional Fourier transform. The neutral limit fε =0.8 implies that there is an imbalance between TKE production and dissipation in the simplified TKE budget equation. Similarly,
we found a production-dissipation imbalance for the temperature fluctuation budget equation. Correcting for the production-dissipation
imbalance, the ‘standard’ MOST functions for dimensionless wind speed and temperature gradients (φm and φm) were determined from fε and fT and compared with the φm and φh formulations of Businger and others. We found good agreement with the Beljaars and Holtslag [J. Appl. Meteorol. 30, 327–341 (1991)] relations. Lastly, the flux and gradient Richardson numbers are discussed also in terms of fε and fT. 相似文献
15.
通过等熵位涡和热力学能量方程的各项诊断对2018年1月上旬我国东部一次寒潮天气过程进行分析,重点给出垂直运动在寒潮降温中的作用。结果表明：此次寒潮天气过程主要受蒙古国南部的横槽转竖影响,巴尔喀什湖东部和西伯利亚地区及其北部为引起这次寒潮的主要冷空气源地。欧亚大陆北部和极区对流层高层和平流层低层的高位涡强冷空气沿着等熵面向南向下平流,引导强冷空气侵袭我国东部。等熵位涡大值区的东侧对应上升运动区,有利于降水的产生。寒潮期间风场平流引起的850 hPa强降温区主要位于东南沿海地区,降温幅度最高可达6×10-4 K·s-1,而东北地区在整个寒潮期间冷平流强度较弱,最大降温幅度仅约为1×10-4 K·s-1。通过计算东南沿海和东北地区区域平均风场平流和垂直运动引起850 hPa温度变化,得出寒潮期间两地的温度总降幅约为1×10-4 K·s-1。东南沿海地区的寒潮主要由风场的冷平流引起,而东北地区则是由冷平流和垂直上升运动的共同作用引起。垂直方向上,东北地区冷空气能影响的高度要远高于东南沿海地区。 相似文献
16.
A model is developed to simulate the potential temperature and the height of the mixed layer under advection conditions. It includes analytic expressions for the effects of mixed-layer conditions upwind of the interface between two different surfaces on the development of the mixed layer downwind from the interface. Model performance is evaluated against tethersonde data obtained on two summer days during sea breeze flow in Vancouver, Canada. It is found that the mixed-layer height and temperature over the ocean has a small but noticeable effect on the development of the mixed layer observed 10 km inland from the coast. For these two clear days, the subsidence velocity at the inversion base capping the mixed layer is estimated to be about 30 mm s–1 from late morning to late afternoon. When the effects of subsidence are included in the model, the mixed-layer height is considerably underpredicted, while the prediction for the mean potential temperature in the mixed layer is considerably improved. Good predictions for both height and temperature can be obtained when values for the heat entrainment ratio,c, 0.44 and 0.68 for these two days respectively for the period from 1000 to 1300 LAT, were used. These values are estimated using an equation including the additional effects on heat entrainment due to the mechanical mixing caused by wind shear at the top of the mixed layer and surface friction. The contribution of wind shear to entrainment was equal to, or greater than, that from buoyant convection resulting from the surface heat flux. Strong wind shear occurred near the top of the mixed layer between the lower level inland flow and the return flow aloft in the sea breeze circulation.Symbols
c
entrainment parameter for sensible heat
-
c
p
specific heat of air at constant pressure, 1010 J kg–1 K–1
-
d
1
the thickness of velocity shear at the mixed-layer top, m
-
Q
H
surface sensible heat flux, W m–2
-
u
m
mean mixed-layer wind speed, m s–1
-
u
*
friction velocity at the surface, m s–1
-
w
subsidence velocity, m s–1
-
W
subsidence warming,oC s–1
-
w
e
entrainment velocity, m s–1
-
w
*
convection velocity in the mixed layer, m s–1
-
x
downwind horizontal distance from the water-land interface, m
-
y
dummy variable forx, m
-
Z
height above the surface, m
-
Z
i
height of capping inversion, m
-
Z
m
mixed-layer depth, i.e.,Z
i–Zs, m
-
Z
s
height of the surface layer, m
-
lapse rate of potential temperature aboveZ
i, K m–1
-
potential temperature step atZ
i, K
- u
h
velocity step change at the mixed-layer top
-
m
mean mixed-layer potential temperature, K 相似文献
17.
This study investigates the organised motion near the canopy-atmosphere interface of a moderately dense spruce forest in heterogeneous,
complex terrain. Wind direction is used to assess differences in topography and surface properties. Observations were obtained
at several heights above and within the canopy using sonic anemometers and fast-response gas analysers over the course of
several weeks. Analysed variables include the three-dimensional wind vector, the sonic temperature, and the concentration
of carbon dioxide. Wavelet analysis was used to extract the organised motion from time series and to derive its temporal scales.
Spectral Fourier analysis was deployed to compute power spectra and phase spectra. Profiles of temporal scales of ramp-like
coherent structures in the vertical and longitudinal wind components showed a reversed variation with height and were of similar
size within the canopy. Temporal scales of scalar fields were comparable to those of the longitudinal wind component suggesting
that the lateral scalar transport dominates. The existence of a – 1 power law in the longitudinal power spectra was confirmed
for a few cases only, with a majority showing a clear 5/3 decay. The variation of effective scales of organised motion in
the longitudinal velocity and temperature were found to vary with atmospheric stability, suggesting that both Kelvin-Helmholtz
instabilities and attached eddies dominate the flow with increasing convectional forcing. The canopy mixing-layer analogy
was observed to be applicable for ramp-like coherent structures in the vertical wind component for selected wind directions
only. Departures from the prediction of m = Λ
w
L
s
−1 = 8–10 (where Λ
w
is the streamwise spacing of coherent structures in the vertical wind w and L
s
is a canopy shear length scale) were caused by smaller shear length scales associated with large-scale changes in the terrain
as well as the vertical structure of the canopy. The occurrence of linear gravity waves was related to a rise in local topography
and can therefore be referred to as mountain-type gravity waves. Temporal scales of wave motion and ramp-like coherent structures
were observed to be comparable. 相似文献
18.
准确估算热带气旋(TC)强度,对于预测TC发展、减少财产损失具有重要的意义。前人将TC看作满足静力平衡和梯度风平衡的轴对称涡旋系统,基于云顶高度、云顶温度、海表面气压等物理量建立了TC强度估算模型,该模型未考虑环境垂直风切变对TC强度的影响。本文提出一种修正模型,通过统计拟合手段将垂直风切变加入原模型中。从2006—2015年的Cloud Sat资料中筛选出穿心个例共63个。针对云雷达(CPR)数据特点,提出根据反射率因子的垂直分布确定眼墙和外围边界位置的方法。分别用原模型与修正模型对这63个TC个例进行强度估算。与最佳路径数据相比,原模型结果总体偏大,尤其对风切变较大、强度较小的个例估算效果不佳。修正模型对于风切变大于5 m·s~(-1)的个例误差明显减小,平均绝对误差MAE、均方根误差RMSE和平均绝对误差百分比MAPE分别从5.8 m·s~(-1)、7.7 m·s~(-1)和19.5%变为3.5 m·s~(-1)、4.9 m·s~(-1)和11.5%。在一定强度范围内,修正模型估算效果随着强度的增强而提升。修正模型对于成熟阶段的个例效果更好,北半球的估算精度高于南半球,纬度越高,估算误差越小。试验结果表明,用该修正模型估算TC强度是可行的,可以对现有的技术进行辅助和补充。 相似文献
19.
The formation mechanism of the nocturnal urban boundary layer (UBL), especially in the winter nighttime, was investigated based on the extensive field observations conducted during November 1984 in Sapporo, Japan. A strong, elevated inversion formed over the Sapporo urban area and the inversion base height was approximately twice the average building height. Velocity fluctuations
u, w and Reynolds stress % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaaca% WG1bWaaWbaaSqabeaacaaIXaaaaGGaaOGae8hiaaIaam4DamaaCaaa% leqabaGaaGymaaaaaaaaaa!3A9C!\[\overline {u^1 w^1 } \] had nearly uniform profiles within the nocturnal UBL and decreased with height above the UBL. On the other hand, temperature fluctuations
t
, and heat fluxes % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaaca% WG1bWaaWbaaSqabeaacaaIXaaaaGGaaOGae8hiaaIaeqiUde3aaWba% aSqabeaacaaIXaaaaaaaaaa!3B56!\[\overline {u^1 \theta ^1 } \] and % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaaca% WG3bWaaWbaaSqabeaacaaIXaaaaGGaaOGae8hiaaIaeqiUde3aaWba% aSqabeaacaaIXaaaaaaaaaa!3B58!\[\overline {w^1 \theta ^1 } \] had peaks at the inversion base and small values within the nocturnal UBL. The turbulent kinetic energy budget showed that the turbulent transport term and shear generation from urban canopy elements are important in the nocturnal UBL development; the role of the buoyancy term is small. The turbulence data analysis and application of a simple advective model showed that the mechanism of UBL formation may be controlled by the downward transport of sensible heat from the elevated inversion caused by mechanically-generated turbulence.Nomenclature
g
accelaration due to gravity, m s-2
-
k
turbulent kinetic energy, m2 s-1
-
K
m
eddy viscosity, m2 s-1
-
L
Monin-Obukhov lenght, m
-
p
pressure, Kg m-2
-
U, V, W
mean wind speed in the downwind, crosswind, and vertical directions, respectively, m s-1
-
u
1, w
1
wind speed fluctuation in the downwind and vertical direction, respectively, m s-1
-
u
1
friction velocity, m s-1
- % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaaca% WG1bWaaWbaaSqabeaacaaIXaaaaGGaaOGae8hiaaIaam4DamaaCaaa% leqabaGaaGymaaaaaaaaaa!3A9C!\[\overline {u^1 w^1 } \]
momentum flux, m2s-2
- % MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaaca% WG1bWaaWbaaSqabeaacaaIXaaaaGGaaOGae8hiaaIaam4DamaaCaaa% leqabaGaaGymaaaaaaaaaa!3A9C!\[\overline {u^1 \theta^1 } \]
sensible heat flux, m2s-1°C
-
WD
wind direction, deg
-
WS
wind speed, m s-1
-
z
altitude, m
-
Z
h
inversion base height, m
-
Z
j
wind maximum height, m
-
Z
t
inversion top height, m
-
T
u-r
heat island intensity, °C
-
temperature lapse rate at rural site, °C m-1
-
energy dissipation rate, m2s-3
-
1
Potential temperature fluctuation, °C
-
*
scaling temperature, (=-% MathType!MTEF!2!1!+-% feaafeart1ev1aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn% hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr% 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9% vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x% fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaa0aaaeaaca% WG1bWaaWbaaSqabeaacaaIXaaaaGGaaOGae8hiaaIaeqiUde3aaWba% aSqabeaacaaIXaaaaaaaaaa!3B56!\[\overline {u^1 \theta ^1 } \]/u*) °C
-
mean potential temperature fluctuation, K
-
density of air, Kgm-3
-
K
von Kármán constant (=0.4)
- u, v, w
standard deviation of wind speed in the downwind, crosswind, and vertical directions, respectively, m s-1
-
standard diviation of temperature, °C 相似文献